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1.
南极中山站冬季电离层的平均特性   总被引:7,自引:3,他引:7       下载免费PDF全文
本文利用南极中山站的数字式电离层垂直测高仪1995年的频高图资料,对中山站上空冬季电离层的一些平均特性进行了初步分析。中山站冬季电离层F层很不稳定,其日变化比较明显,foF2的月中值在0900UT出现极大并在1400UT附近出现次极大。最大值在0900UT(磁中午)附近,这是极隙区软电子沉降、极区等离子体对流和光辐射电离效应等诸多因素综合作用的结果,形成了所谓的磁中午异常。在2000~0100UT之间foF2数值较小,可能是由于这段时间中山站正处于电离层极洞区域。Es层几乎每天都可以观测到,在1700UT附近出现机率较高,并且foEs数值较大,多数为极光型Es,主要是由于极光粒子沉降引起的。电离层E层的变化相对平缓。  相似文献   

2.
MeanionosphericpropertiesinwinteratZongshanStation,AntarcticaTX@刘顺林@贺龙松@刘瑞源MeanionosphericpropertiesinwinteratZhongshanStation,An...  相似文献   

3.
南极中山站的f_0F2特征   总被引:3,自引:0,他引:3       下载免费PDF全文
本文利用电离层数字测高仪 (DPS - 4)所测的f0 F2和从美国NOAA和DMSP卫星观测估算的半球功率指数和午夜极光区赤道侧边界纬度等资料 ,考察中山站电离层的极区特征。结果表明 ,冬季中山站电离层内的电离生成主要取决于从磁层沉降的粒子。在太阳活动和地磁变化宁静环境下 ,磁正午极隙区内的软粒子是最主要的电离源 ,它能使f0 F2达全天的最大值 ;上、下午各有数小时处于极光带内时 ,高能粒子的电离作用也很重要 ;夜间进入极盖区后 ,电子密度则很低。夏季太阳辐射电离效应使f0 F2值比冬季增加 1- 1 .5MHz,而其日变化的最大值时间也提前了 1- 2hr。发生很大扰动时 ,极隙区和极光带的位置均向低纬方向移动。若中山站日间也处于极盖区内时 ,电子密度会大幅度下降 ,并常接收不到电离层回波的信号。在中等扰动环境下情况更加复杂。由于高纬电离层对流速度很高 ,离子 /中性分子间的碰撞复合系数就很大。热层中性大气全球经向环流对高纬电离层电子密度的增加无显著作用。磁暴期间中午从极隙区向南的等离子体对流对中山站f0 F2的增高也无明显影响。  相似文献   

4.
杨少峰  刘勇华 《极地研究》1999,10(2):155-162
In this paper the data of geomagnetic pulsations at Zhongshan Station from February 3 to Novernber 30 in 1996 are analyzed in ordcr to study polarization characteristics of Zhongshan Station Pc3 pulsations which comprises the cusp Pc3 pulsation and the nightside Pc3 pulsation. For the cusp Pc3 pulsation. the right-handed polarization is always dominant. But their orientation of major axes of polarizations changes with season, NW-SE is dominant in summer and NE-SW in winter. For the nightside Pc3 pulsation,the right-handed with NE-SW is always dominant before midnight. But the left-handed with the mixing orientation of major axes is dominant in summer and the NE-SW with the mixing polarization sense is dominant in winter after midnight. It means that the two types of Zongshan Station Pc3 pulsations have different sources.  相似文献   

5.
The auroral occurrence over Zhongshan Station, Antarctica   总被引:1,自引:0,他引:1       下载免费PDF全文
The auroral data observed by all sky TV camera during 1995 and 1997 at Zhongshan Station of Antarctica are used to analyze the statistic characteristics of the aurora over Zhongshan Station. Around postnoon (1200 - 1600UT ) and midnight (2000 - 0100 UT ), the aurora appears more frequently and stronger than those in evening (1600- 2000UT ). The corona type auroras mainly occur at poleward and overhead of Zhongshan Station during postnoon and around midnight. The hand type auroras mainly appear during postnoon. while during evening and around midnight only appear at equatorward. The active surges mostly appear around midnight,while the transpolar arcs mainly occur after midnight. Except for the transpolar arcs. the occurrences of the other three type auroras are related with Kp index. Usually Zhongshan Station enters the auroral oval at postnoon,the exact time depends on Kp index.  相似文献   

6.
Ionograms, which were obtained from February 1995 to January 1999 by a Digisonde Portable Sounder-4 (DPS-4) at Zhongshan Station in Antarctica, have been scaled. The ionograms interpretation has shown various ionosphcric phcnomena occurred in the cusp region. They are particle precipitation effects in the E region. F region magnetic noon phenomena, slant Es phenomena and lacuna. F layer irregularity zone (FLIZ) phenomena, and auroral oval identification. Typical examples of ionograms and ionogram sequences observed at Zhongshan Station are displayed in this paper.  相似文献   

7.
In the paper the high latitude ionospheric absorption events, monitored by an imaging riometer at Zhongshan Station, Antarctica, are examined during magnetic storms in early May, 1998. The storm absorption at ~0639 UT on May 2 was mainly an equatorward progressing absorption event, which were associated with a strong negative bay of the magnetic H component and with a large Pc3 range pulsation. There was a time lag of about 1. 5 hours between the onset of the ionospheric disturbance and the IMF southward turning in the solar wind. The event at 2222 UT on May 2 was a typical midnight absorption spike event. The absorption region took the form of an elongated strip with the length of 100 - 150 km and the width of 30 - 40 km. The absorption during 0830 - 1200 UT on May 6 was a polar cap absorption (PCA) event,caused by intense precipitation of high-energy protons erupted after a large solar flare explosion.  相似文献   

8.
甄卫民  曹冲  吴健 《极地研究》1994,5(2):53-57
AnalysisoftheionosphericanomalyatGreatWallStation,AntarcticaZhenWeimin(甄卫民);CaoChong(曹冲)andWuJian(吴健)(ChinaResearchInstituteo...  相似文献   

9.
Using the ground observation data at Zhongshan Station of Antarctica during July 13 to 17, 2000, the intense absorption events associated with the activities of the solar active region R9077 are analyzed. It was shown that an intense polar cap absorption event lasted more than 3 days, which was caused by the solar proton event associated with the X5/3B major flare at 1024 UT on July 13. The polar cap event started at about 1040 UT on July 14, and lasted to about 1940 UT on July 17, with a typical day night variation. At the same time, the intense solar activities extremely disturbed the magnetosphere, therefore aurora substorms occurred frequently. The energetic particle precipitation from the magnetosphere caused several absorption spikes superposing on the background of polar cap absorption. One distinct event is the absorption enhancement that started at about 0300 UT on July 15, reached its peak of 26 dB at about 0645 UT and recovered at about 1110 UT on the same day, which was the strongest absorption event observed at Zhongshan Station since the imaging riometer installed in February, 1997. Another outstanding absorption spike with pulsation occurred at about 1753 UT on 14th, its peak reached to 6 dB.  相似文献   

10.
利用南极地磁资料研究了地磁扰日变化SD场特征。1)SD场变化不如Sq场变化规则,无明显的昼夜差异;太阳活动高年(1991年)比下降年(1994年)SD场变化更强烈。2)极隙区中山站SD场变幅比亚极光区长城站和北半球低纬区北京台的SD场变幅大10倍以上。3)中山站S0D(H)变化呈“正弦波”形态,与长城站和北京台S0D(H)变化形态相反。4)中山站S0D等效电流矢量在早晨-下午(02~15h)矢量方向为反时针西向,下午-夜间(15~02h)矢量方向为顺时针东向,这是由极区东向、西向电射流和极区电流涡旋所引起;长城站与北京台S0D等效电流矢量很小,这是由极区东向和西向电射流的影响所致。  相似文献   

11.
在南极中山站使用TD-4A测高仪,从1990年3月至今已取得了10万余帧的电离图记录。由于中山站处在极尖区附近这样一个特殊位置,所以这些电离图能显示出大多数高纬现象,诸如极光卵现象、FLIZ(F层不均匀区)现象、倾斜Es和空白现象、F区磁纬中午现象、E和D区的粒子沉降效应,以及粒子E层(夜间E层)现象等。本文对这些现象进行了描述和初步分析。  相似文献   

12.
何昉  张北辰 《极地研究》2011,23(3):159-167
利用2006-2007年EISCAT Svalbard雷达(ESR)和南极中山站DPS-4测高仪的观测数据,对太阳活动低年不同季节的极区电离层F2层临界频率(f0F2)和峰值高度(hmF2)进行统计分析,研究其日变化特征,并与国际参考电离层IRI-2007模式比较.结果表明,在太阳活动低年,夏季两站的观测结果与IRI预...  相似文献   

13.
本文通过 1 997年在南极中山站观测的极光和所对应的地磁场扰动 ,利用 AU、AL、AE指数描述极光电集流在南极中山站的分布规律及其强度 ,我们发现东向极光电集流强度是正值 ,西向极光电集流强度是负值 ,从绝对值来说 ,西向极光电集流强度大于东向极光电集流强度。南极中山站夏季的极光电集流强度大于冬季的极光电集流。秋夏冬季节的东向极光电集流在72 0~ 1 44 0分 (世界时 1 2~ 2 4时 )的分布规律的拟合曲线类似口朝上的抛物线形 ;西向极光电集流在 72 0~ 1 44 0分这段时间的分布规律的拟合曲线类似正弦波形。了解了极光电集流在南极中山站的分布特征 ,有利于极区电离层和磁层耦合及极光动力学的研究。  相似文献   

14.
甄卫民  曹冲  吴健 《极地研究》1994,6(3):36-40
本文采用现有模式,利用长城站电离层观测资料,模拟计算了F2层峰值高度及子午向热层风昼夜变化等。同时采用了热层风模式计算了长城站热层风的经验预测值。计算结果较好地解释了长城站的两个异常特征。夏季异常即f0F2最大值出现在夜间。冬季特别是6、7月份临频显著减小。太阳辐射电离与热层中性风的竞相联合作用是导致夏季异常的关键。长城站地理上虽属高纬区,却处在地磁中纬区,这是分析上述异常特征中需要考虑的一个重要因素  相似文献   

15.
利用中山站1995-2006年的电离层垂测数据统计分析了当地电离层F2层峰值电子浓度(NmF2)对太阳活动变化的依赖性,研究发现在中山站NmF2月中值随修正太阳10.7厘米通量指数F10.7P增大而增大,其饱和或放大趋势不明显。除冬季12-16 UT、20-2 UT与夏季2-11 UT以外的绝大部分时刻,两者具有良好的线性关系。NmF2月中值随F10.7P变化斜率随季节、地方时而变化。在日变化中,NmF2随F10.7P变化斜率极大值出现在磁中午附近,明显大于其他时刻,在夜侧变化斜率整体较小,且在分季和冬季的夜侧以及夏季全天,其斜率随地方时变化不大。在年变化中,日侧斜率最大值出现在两分季,冬季次之,夏季最小;而夜侧斜率在夏半年(10月-3月)整体上要大于冬半年(4月-9月)。结合中山站位于极隙区纬度的特殊地理位置,分析了上述NmF2变化特征的可能原因。  相似文献   

16.
南极中山站地磁脉动的观测分析   总被引:1,自引:0,他引:1       下载免费PDF全文
本文分析的是1992年2月9日至1993年2月9日在南极中山站记录的各种地磁脉动的观测资料,并对各种地磁脉动的激发机制进行了初步讨论。通过南极中山站地磁脉动观测资料分析,了解高纬地区地磁脉动的形态特征,对南极极隙区高空大气电磁环境、太阳风和磁层相互作用等现象有进一步的认识。  相似文献   

17.
中国南极新站选择在维多利亚地特拉诺瓦湾难言岛上进行建设,其气象环境状况是开展科学研究的基础工作,也是考察队员生命安全保障的基础资料。因此,通过2013年度难言岛气象站的观测资料,结合附近地区历史气象资料,对该区域气象要素特征进行了分析。结果表明:(1)由于地处罗斯海与东南极冰盖交界处,难言岛年均气压为987.8 h Pa,与中山站非常接近;(2)年均温为-16.1℃,最低气温为-39.3℃,且冬季气温波动较大,标准差可达±6.0℃;(3)年均相对湿度为42.1%,年均比湿为0.6 g·kg-1且冬季比湿极低,空气非常干燥,降水量非常低;(4)盛行风向为WNW,5—7级风出现频率超过50%,但夏季风速明显低于冬季风速,一般不超过8.0 m·s~(-1),有利于中国在夏季开展工程建设和补给;(5)难言岛年总辐射量为3 342.8 MJ·m~(-2),明显低于中山站,但两站反照率非常接近。  相似文献   

18.
南极中山站极光形态的统计特征   总被引:9,自引:4,他引:5       下载免费PDF全文
利用极光全天空摄象机1995年和1997年在南极中山站观测的极光数据,对中山站上空极光的出现情况进行了统计分析。在南极中山站,午后(磁地方时1400~1800MLT)和子夜前后(2200~0300MLT)出现极光的情况比较多,在傍晚(1800~2200MLT)出现极光的情况要少一些;较强的极光主要也出现在午后和子夜附近。冕状极光主要出现在子夜附近和午后的极向侧和天顶,在傍晚出现很少;带状极光主要出现在午后和赤道侧的傍晚与子夜;极光浪涌主要出现在子夜前后;向日极光弧则主要出现在子夜前后,子夜前比子夜后多,极向和天顶比赤道侧多。除向日极光弧外,其它形态的极光在中山站的出现情况与Kp指数相关。中山站进入极光带的时间通常在午后,具体时间也与Kp指数有关  相似文献   

19.
Two induction magnetometers have been installed at Chinese Zhongshan Station and Australia Davis Station, Antarctica respectively. We adopt the cross spectral analysis technique to analyze the data of the two induction magnetometers, in June, September, December 1996 and March 1997, and to investigate Pc5 frequency range pulsation (150 600 s) occurrence and propagation in cusp latitude. The results are summarized as follows: At Zhongshan Davis Station, the magnetic pulsations in Pc5 frequency band can occurs over a wide time, but more frequently at pre local magnetic noon and pre local magnetic midnight. The Pc5 pulsations have no significant seasonal variation in the amplitude, occurrence and propagation. The amplitude has a small peak at pre local magnetic noon and large value sometimes at pre local magnetic midnight. In daytime, the Pc5 pulsations propagate westward in morning and eastward in afternoon, and reversal at local magnetic noon. In nighttime, the Pc5 pulsations propagate westward before 20:00 MLT and eastward after 20:00 MLT. Near dusk time, the Pc5 pulsations propagate irregularly. These characteristics indicate that the Pc5 pulsations have different source at different local magnetic time.  相似文献   

20.
极隙区Pc3频段脉动的传播特性   总被引:1,自引:0,他引:1       下载免费PDF全文
南极中山站和戴维斯站 (不变磁纬 74.5°S)白天中午位于磁层极隙区 ,夜间位于极盖区或极光带的极向边沿。两站均安装了完全相同的感应式磁力计。选择两站 1 997年 3月和 1 996年 6、9、1 2月的数据 ,运用快速傅立叶变换和波形检查方法选择 Pc3频段脉动事件 ,然后用信号互谱技术进行统计分析 ,结果如下 :在中山站 -戴维斯站 ,Pc3频段脉动主要出现于白天中午 /磁中午和磁午夜附近 ;白天 ,Pc3频段脉动振幅、出现率和出现的时间范围均有一定的季节变化 ,冬季最小 ,但在夜间 ,Pc3频段脉动没有这种变化 ;夜间 ,Pc3频段脉动振幅比在白天大许多 ;Pc3频段脉动传播方向 ,白天主要向西 ,夜间不太规则。这些可能反映了电离层电导率和日侧电离层电流系统对 Pc3频段脉动的影响。  相似文献   

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